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Anomalous Nonlinear Dynamics Behavior of Fractional Viscoelastic Beams
Author(s) -
Jorge L. Suzuki,
Ehsan Kharazmi,
Pegah Varghaei,
Maryam Naghibolhosseini,
Mohsen Zayernouri
Publication year - 2021
Publication title -
journal of computational and nonlinear dynamics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.606
H-Index - 48
eISSN - 1555-1423
pISSN - 1555-1415
DOI - 10.1115/1.4052286
Subject(s) - nonlinear system , fractional calculus , viscoelasticity , mathematical analysis , partial differential equation , physics , ordinary differential equation , mathematics , classical mechanics , differential equation , equations of motion , vibration , bifurcation , quantum mechanics , thermodynamics
Fractional models and their parameters are sensitive to intrinsic microstructural changes in anomalous materials. We investigate how such physics-informed models propagate the evolving anomalous rheology to the nonlinear dynamics of mechanical systems. In particular, we study the vibration of a fractional, geometrically nonlinear viscoelastic cantilever beam, under base excitation and free vibration, where the viscoelasticity is described by a distributed-order fractional model. We employ Hamilton's principle to obtain the equation of motion with the choice of specific material distribution functions that recover a fractional Kelvin–Voigt viscoelastic model of order α. Through spectral decomposition in space, the resulting time-fractional partial differential equation reduces to a nonlinear time-fractional ordinary differential equation, where the linear counterpart is numerically integrated through a direct L1-difference scheme. We further develop a semi-analytical scheme to solve the nonlinear system through a method of multiple scales, yielding a cubic algebraic equation in terms of the frequency. Our numerical results suggest a set of α-dependent anomalous dynamic qualities, such as far-from-equilibrium power-law decay rates, amplitude super-sensitivity at free vibration, and bifurcation in steady-state amplitude at primary resonance.

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